Apparatus and method for federal reserve note authentication

Abstract: A detection system for detecting and/or verifying the magnetic properties of the magnetic ink layer in Federal Reserve Notes or other documents includes, in order of interaction with the magnetic ink of a Note, a saturation record head, a saturation read head, a non-saturation record head, and a non-saturation read head. The disclosed method of operation is equivalent to the normal testing of the magnetic layer of a Note, but eliminates the need for an erase magnet.

Description: Field of Invention This invention relates generally to the detection of magnetic fields and, more particularly to the detection of and/or verification of the magnetic fields associated with Federal Reserve Note currency such as it is, for example, known from US-A-4 587 412. Federal Reserve Notes are printed, in part, with a magnetic ink which provides each Note with a detectable magnetic layer. Background of the Invention In the related art, the magnetic field detection system used for the detection and verification of Federal Reserve Note currency uses a 5-head process shown in Fig. 1. A Federal Reserve Note 11 is transported in a direction shown by the Arrow in Fig. 1. The Note 11 first encounters a high frequency erase head 15. The high frequency erase head 15 demagnetizes the magnetic ink on the Federal Reserve Note. Next the Note 11 is passed over a non-saturation record head 16 where the Note 11 is exposed to a field that magnetizes the ink to approximately 80% of saturation. The Note is next passed over non-saturation read head 17, the non-saturation read head detecting a remanent moment resulting from the application of the non-saturation magnetic field. The Note 11 is next passed over a saturation record head 18 which provides a field which magnetizes the magnetic ink layer to saturation. Finally, the Note 11 is passed over a saturation read head 19 which detects the saturation remanence moment resulting from application of the saturation magnetic field. The operation of the prior art testing method can be understood by reference to Fig. 2. Fig. 2 is a plot of the magnetization of the material versus the magnetic field, commonly called the hysteresis loop. The Note 11 first has an erase field applied thereto which results in the magnetic layer having the magnetic properties identified by point 21 of Fig. 2. When a non-saturation (80%) magnetic field is applied to the Note 11, the magnetic layer has the properties associated with a point 22 relative to the hysteresis curve 20. When the Note 11 is moved from the vicinity of the non-saturation magnetic field head, the magnetic properties (remanence moment) assume the properties defined by point 23. This remanence moment defined by point 23 is measured by the non-saturation magnetic field read head 17. Note 11 is then subjected to a saturation magnetic field and the field in the magnetic layer is shown by point 24 of Fig. 2. Once removed from the saturation magnetic field record head 18, the remanence magnetization at point 25 is measured by the saturation magnetic field read head 19. The measurements of the remanence field at point 23 and point 25 are used to authenticate the Note 11. The conventional magnetic ink detection apparatus described above requires an erase head. A conventional erase head consists of a gapped magnetic core wound with many turns of wire. The wire carries a high frequency A.C. field. When the Note passes in the vicinity of the gap in the core, the Note is subject to a large alternating polarity magnetic field. The magnetic field experienced by the Note decays to zero as the Note moves away from the gap. The large alternating field erases any preexisting magnetization that can be present in the Note. As a result of the application of the decaying large alternating field, the layer of the Federal Reserve Note is at point 21 of Fig. 2. In certain apparatus used in the scanning of the Federal Reserve Notes, a ± 1 mm tolerance in the Note to erase head separation is established and the Notes are scanned at 10 m/sec. In order to erase the preexisting magnetic field effectively, the A.C. erase field must be very large and be modulated with a high frequency. This large, high frequency field generates a significant noise signal in the read heads 17 and 19 of Fig. 1. The result of the generated noise, is that the signal to noise ratio is lowered. Because of the large, high frequency current flowing in the turns of wire of the erase head, an unacceptable power can be dissipated by the erase head and excess heating can occur. A need has therefore been felt for apparatus and a procedure which can eliminate the need for the erase magnet in a Federal Reserve Note magnetic ink detection system. Summary of the Invention The present invention is directed to overcoming one or more of the problems set forth above. Briefly summarized, according to one aspect of the present invention, the apparatus for detecting the magnetic ink in Federal Reserve Note currency includes, in the sequence with which the apparatus interacts with the Note, a saturation record head, a saturation read head, a non-saturation record head and a non-saturation read head. By proper selection of the fields applied to the Note, this procedure can provide information equivalent to the information provided by the prior art technique, but, however, without the need for an erase head. These and other aspects, objects, features and advantages of the present invention will be more clearly understood and appreciated from a review of the following detailed description of the preferred embodiments and appended claims, and by reference to the accompanying drawings. The present invention permits the magnetic ink in a Federal Reserve Note to be detected and/or verified without requiring a bulky, noisy and power-consuming erase head. Brief Description of the Drawings Figure 1 is a block diagram of a magnetic field detection system used for the verification of currency according to the related art. Figure 2 illustrates the procedure for measuring parameters of a layer of magnetic material according to the prior art. Figure 3 is a block diagram of a magnetic field detection system according to the present invention. Figure 4 illustrates the procedure for measuring parameters of a layer of magnetic material according to the present invention. Figure 5 is a more detailed block diagram of the preferred embodiment of the detection system according to the present invention. Detailed Description of the Invention Referring to Fig. 3, the detection system for the detection of the magnetic ink in a Federal reserve Note is shown. The detection system includes a saturation record head 31 which is the first element of the detection system to interact with the Note 11. The second element of the detection system to interact with the Note 11 is a saturation read head 32. Then, the interaction occurs with a non-saturation record head 33 and finally, the detection system interacts with the Note 11 by means of a non-saturation read head 34. As indicated above, the prior art procedure for the determination of the magnetic properties of a magnetic layer is to erase the magnetic moment of the Note and then apply a magnetic field which is 80% of the saturation field. After application of this 80% field, the magnetic moment is measured. In the present invention, equivalent information can be obtained by applying a saturation field and then applying an opposite polarity magnetic field to the layer which is equivalent to the application of 80% (of saturation) magnetic field applied to the layer which has been erased. The basis of operation of the present invention is that, for low magnetic particle concentrations such as those found on a Federal Reserve Note, the magnetizing and demagnetizing particle switching field distributions are the same. The equivalence is expressed by the following (Wohlfarth) equation; -M d (H) = 2M r (H) - M rs where M r (H) is the remanent moment starting from zero, M d (H) is the demagnetizing remanent moment starting from -M rs , and M rs is the saturation remanence of the particle assembly. Equation 1 can be written; M r (H) = ½ [M rs - M d (H)] or M r /M rs = ½ (1 - M d /M rs ). From Equation 3, when M r (H)/M rs = 0.8 , then M d (H)/M rs = -0.6 . Therefore, if one applies a field large enough to provide M d /M rs = -60% , this is equivalent to M r /M rs = 80% . The operation of the magnetic head array, according to the present invention, can be understood by reference to Fig. 4. The saturation field magnetic head causes the magnetization M in the magnetic layer to reach a point 41 on hysteresis curve 40. When the Note is removed from the vicinity of the saturation record head, the saturation remanence field, measured by the saturation magnetic field read head is determined by point 42. The Note is moved to the vicinity of the non-saturation record head where the field in the magnetic layer and the magnetization are determined by point 43 on the hysteresis loop 40. When the Note is removed from the vicinity of the non-saturation record head, the non-saturation read head measures the remanence at point 44. This remanence is related to the remanence of the prior art procedure in the manner described above in Equation 3. The magnetic moment M rs , measured by the saturation read head 32 of Fig. 3, and the demagnetizing magnetic moment measured by the non-saturation read head 34 of Fig. 3, are of opposite polarity, i.e., 180° out of phase, when the Note is genuine. When a counterfeit Note is tested and the counterfeit Note has a high coercivity, i.e., is resistant to demagnetization, the moment of the counterfeit note can be reduced to the proper 60% of saturation, but is not reversed in polarity. Provision can be made in the signal reproduction electronics to detect the phase of the non-saturated signal as well as its magnitude. In this manner, high coercivity counterfeit Notes can be identified and eliminated. Referring to Fig. 5, the configuration for the preferred embodiment of the magnetic head array is shown. A first combined head 50 includes elements 51 for producing the saturation magnetic field, a sensor 52 in the gap of elements 51 for detecting the saturation magnetic field, and a saturation read head 53 for detecting the remanent moment in the magnetic layer produced by the elements 51. The elements 51 include a permanent magnet 51A between soft magnetic material yokes. A second combined head 55 includes elements 56 for providing a non-saturating magnetic field in a direction opposite direction to that of the from the field of the first combined head, a sensor 57 located in the gap of the field producing elements 56 and a sensor 58 for detecting the remanence moment of the magnetic layer resulting the interaction of the first combined head 50 and second combined head 55. The elements 56 include a permanent magnet 56A between soft magnetic material yokes. The extra "in-field" detectors 52 and 57 of Fig. 5 measure the magnetization of the Note at points 41 and 43 of Fig. 4 and provides additional information to aid in the authentication. The sensing principle of detectors 52 and 57 is that of magneto resistance. Thin films of 81/19 NiFe are located in the gaps of structures 51 and 56 so that the plane of the films are perpendicular to the large magnetic field at those points. Because the plane of the film is perpendicular to the large field, this field is not detected and the sensors can respond to the very small magnetic field emanating from the Notes with excellent signal to noise ratio. The other sensors 53 and 58 of Fig. 5 are also magneto-resistive sensors in the preferred embodiment. While the invention has been described with particular reference to a preferred embodiment, it will be understood by those skilled in the art that various changes may be made and equivalents may be substituted for elements of the preferred embodiment without departing from invention. In addition, many modifications may be made to adapt to a particular situation and material to a teaching of the invention without departing from the essential teachings of the present invention. For example, while the verification of Federal Reserve Notes has been emphasized, it will be clear that this technique can be applied to any magnetic layer. As is evident from the foregoing description, certain aspects of the invention are not limited to the particular details of the examples illustrated, and it is therefore contemplated that other modifications and applications will occur to those skilled in the art. It is accordingly intended that the claims shall cover all such modifications and applications as do not depart from the scope of the invention as defined by the appended claims.

Claims: A magnetic head array for detecting magnetic hysteresis properties of a magnetic layer, said array comprising: as a first element of the detection array a first record head (31) producing a D.C. magnetic field in said magnetic layer, said D.C. magnetic field having a strength sufficient to saturate said magnetic layer in a first direction; a first read head (32) positioned proximate to and downstream from said first record head, said first read head detecting the phase and magnitude of remanent magnetization in said layer produced by said first record head; a second record head (33) located proximate to and downstream from said first read head, said second record head producing a magnetic field in said magnetic layer which is opposite in direction to said D.C. magnetic field produced by said first record head, said magnetic field produced by said second record head being lower in magnitude so as to reverse and partially erase said magnetization recorded by said first record head; and a second read head (34) located proximate to said second record head, said second read head detecting a phase and magnitude of a remanent magnetization remaining in said magnetic layer after passing said second record head. The magnetic head array of claim 1 wherein said first record head includes apparatus for detecting a phase and amplitude of a signal produced by said magnetic layer while said magnetic field is being applied to said magnetic layer. The magnetic head array of claim 2 wherein said first record head is formed by a magneto resistive magnetic field sensing element. The magnetic head array of claim 2 wherein a magneto motive force required to produce a magnetic record field is provided by a permanent magnet in the back region of a yoke constructed from a soft magnetic material. The magnetic head array of claim 1 wherein said first and said second read heads include a magneto resistive magnetic field sensor. The magnetic head array of claim 1 wherein said second record head is adapted to reverse the polarity and partially erase the magnetization of said magnetic layer, said second record head being adapted to detect a phase and a magnitude of the field produced by said magnetization in said magnetic layer. A magnetic head array for detecting magnetic hysteresis properties of a magnetic layer, said array comprising: as a first element of the detection array a first magnetic record head (50) producing a D.C. magnetic field in the magnetic layer, said magnetic field being selected to saturate said magnetic layer in a first direction; a second record head (55) located proximate said first record head, said second record head producing a magnetic field in said layer which is opposite in direction to the magnetic field produced by said first magnetic record head, said magnetic field produced by said second record head having an amplitude sufficient to reverse the polarity and to erase partially or to reverse the magnetization recorded by said first record head; wherein both said first and said second record heads are adapted to simultaneously detect a phase and a magnitude of said magnetization on said magnetic layer. The magnetic head array of any of the preceding claims wherein said magnetic layer is the magnetic ink on a Federal Reserve Note. A method for measuring magnetic hysteresis properties of a magnetic material layer, said method comprising the steps of: firstly saturating the magnetic material layer in a first direction with a saturation magnetic field; measuring a saturation remanence of the layer after removal of the saturation magnetic field; applying a non-saturation magnetic field having a predetermined value and a direction opposite to said saturation magnetic field; and measuring a magnitude and polarity of a non-saturation remanence of the magnetic layer after removal of the non-saturation magnetic field. The method of claim 9 further comprising the step of: comparing a magnitude and a phase of said saturation remanence value with a magnitude and a phase of said non-saturation remanence value.

Inventors: JEFFERS FREDERICK J, JEFFERS, FREDERICK J., JEFFERS, FREDERICK J., C/O EASTMAN KODAK COMPANY
Applicants: EASTMAN KODAK CO, EASTMAN KODAK COMPANY
Application year: 1994
Main classification: G01R33
IPC codes: G06K7, G07D7, G01R33, G01V3, G07F7